Puneet Varma (Editor)

Doob decomposition theorem

Updated on
Edit
Like
Comment
Share on FacebookTweet on TwitterShare on LinkedInShare on Reddit

In the theory of stochastic processes in discrete time, a part of the mathematical theory of probability, the Doob decomposition theorem gives a unique decomposition of every adapted and integrable stochastic process as the sum of a martingale and a predictable process (or "drift") starting at zero. The theorem was proved by and is named for Joseph L. Doob.

Contents

The analogous theorem in the continuous-time case is the Doob–Meyer decomposition theorem.

Statement of the theorem

Let (Ω, F, ℙ) be a probability space, I = {0, 1, 2, . . . , N} with N ∈ ℕ or I = ℕ0 a finite or an infinite index set, (Fn)nI a filtration of F, and X = (Xn)nI an adapted stochastic process with E[|Xn|] < ∞ for all nI. Then there exists a martingale M = (Mn)nI and an integrable predictable process A = (An)nI starting with A0 = 0 such that Xn = Mn + An for every nI. Here predictable means that An is Fn−1-measurable for every nI {0}. This decomposition is almost surely unique.

Corollary

A real-valued stochastic process X is a submartingale if and only if it has a Doob decomposition into a martingale M and an integrable predictable process A that is almost surely increasing. It is a supermartingale, if and only if A is almost surely decreasing.

Remark

The theorem is valid word by word also for stochastic processes X taking values in the d-dimensional Euclidean space d or the complex vector space d. This follows from the one-dimensional version by considering the components individually.

Existence

Using conditional expectations, define the processes A and M, for every nI, explicitly by

and

where the sums for n = 0 are empty and defined as zero. Here A adds up the expected increments of X, and M adds up the surprises, i.e., the part of every Xk that is not known one time step before. Due to these definitions, An+1 (if n + 1 ∈ I) and Mn are Fn-measurable because the process X is adapted, E[|An|] < ∞ and E[|Mn|] < ∞ because the process X is integrable, and the decomposition Xn = Mn + An is valid for every nI. The martingale property

E [ M n M n 1 | F n 1 ] = 0     a.s.

also follows from the above definition (2), for every nI {0}.

Uniqueness

To prove uniqueness, let X = M' + A' be an additional decomposition. Then the process Y := MM' = A'A is a martingale, implying that

E [ Y n | F n 1 ] = Y n 1     a.s.,

and also predictable, implying that

E [ Y n | F n 1 ] = Y n     a.s.

for any nI {0}. Since Y0 = A'0A0 = 0 by the convention about the starting point of the predictable processes, this implies iteratively that Yn = 0 almost surely for all nI, hence the decomposition is almost surely unique.

Proof of the corollary

If X is a submartingale, then

E [ X k | F k 1 ] X k 1     a.s.

for all kI {0}, which is equivalent to saying that every term in definition (1) of A is almost surely positive, hence A is almost surely increasing. The equivalence for supermartingales is proved similarly.

Example

Let X = (Xn)n∈ℕ0 be a sequence in independent, integrable, real-valued random variables. They are adapted to the filtration generated by the sequence, i.e. Fn = σ(X0, . . . , Xn) for all n ∈ ℕ0. By (1) and (2), the Doob decomposition is given by

A n = k = 1 n ( E [ X k ] X k 1 ) , n N 0 ,

and

M n = X 0 + k = 1 n ( X k E [ X k ] ) , n N 0 .

If the random variables of the original sequence X have mean zero, this simplifies to

A n = k = 0 n 1 X k     and     M n = k = 0 n X k , n N 0 ,

hence both processes are (possibly time-inhomogenious) random walks. If the sequence X = (Xn)n∈ℕ0 consists of symmetric random variables taking the values +1 and −1, then X is bounded, but the martingale M and the predictable process A are unbounded simple random walks (and not uniformly integrable), and Doob's optional stopping theorem might not be applicable to the martingale M unless the stopping time has a finite expectation.

Application

In mathematical finance, the Doob decomposition theorem can be used to determine the largest optimal exercise time of an American option. Let X = (X0, X1, . . . , XN) denote the non-negative, discounted payoffs of an American option in a N-period financial market model, adapted to a filtration (F0, F1, . . . , FN), and let denote an equivalent martingale measure. Let U = (U0, U1, . . . , UN) denote the Snell envelope of X with respect to . The Snell envelope is the smallest -supermartingale dominating X and in a complete financial market it represents the minimal amount of capital necessary to hedge the American option up to maturity. Let U = M + A denote the Doob decomposition with respect to  of the Snell envelope U into a martingale M = (M0, M1, . . . , MN) and a decreasing predictable process A = (A0, A1, . . . , AN) with A0 = 0. Then the largest stopping time to exercise the American option in an optimal way is

τ max := { N if  A N = 0 , min { n { 0 , , N 1 } A n + 1 < 0 } if  A N < 0.

Since A is predictable, the event {τmax = n} = {An = 0, An+1 < 0} is in Fn for every n ∈ {0, 1, . . . , N − 1}, hence τmax is indeed a stopping time. It gives the last moment before the discounted value of the American option will drop in expectation; up to time τmax the discounted value process U is a martingale with respect to .

Generalization

The Doob decomposition theorem can be generalized from probability spaces to σ-finite measure spaces.

References

Doob decomposition theorem Wikipedia


Similar Topics